Difference between revisions of "Linear Hardening"

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=== Hardening and Softening ===
=== Hardening and Softening ===


As implied by the name "Linear Hardening", the law normally models a response where the yield strength increases with plastic strain <math>\alpha</math>. In other words, <math>E_p=\ge 0</math> and <math>K\ge0</math>. This law can also be used to model linear softening by entering a negative modulus. Entry of a negative <math>E_p</math>, however, has to be done by entering a negative <math>K</math>. This entry will result in <math>E_p=K \sigma_{Y0}</math>. Softening will be unstable if is crosses entire cross section of a material under applied load, but is usually stable otherwise or when localized to a yield zone. To prevent non-physical negative values are large plastic strain, the softened yield stress must be limited to a minimum yield stress value (the default minimum is zero).
As implied by the name "Linear Hardening", the law normally models a response where the yield strength increases with plastic strain <math>\alpha</math>. In other words, <math>E_p\ge 0</math> and <math>K\ge0</math>. This law can also be used to model linear softening by entering a negative modulus. Entry of a negative <math>E_p</math>, however, has to be done by entering a negative <math>K</math>. This entry will result in <math>E_p=K \sigma_{Y0}</math>. Softening will be unstable if is crosses entire cross section of a material under applied load, but is usually stable otherwise or when localized to a yield zone. To prevent non-physical negative values are large plastic strain, the softened yield stress must be limited to a minimum yield stress value (the default minimum is zero).


== Hardening Law Properties ==
== Hardening Law Properties ==

Revision as of 13:02, 25 April 2017

In the linear hardening law, the yield stress is given by

      [math]\displaystyle{ \sigma_y = \sigma_{Y0} + E_p\alpha = \sigma_{Y0}(1+K\alpha) }[/math]

where [math]\displaystyle{ \sigma_{Y0} }[/math] is initial yield stress, Ep is the plastic modulus, α is cumulative equivalent plastic strain, and K is a hardening coefficient.

Hardening and Softening

As implied by the name "Linear Hardening", the law normally models a response where the yield strength increases with plastic strain [math]\displaystyle{ \alpha }[/math]. In other words, [math]\displaystyle{ E_p\ge 0 }[/math] and [math]\displaystyle{ K\ge0 }[/math]. This law can also be used to model linear softening by entering a negative modulus. Entry of a negative [math]\displaystyle{ E_p }[/math], however, has to be done by entering a negative [math]\displaystyle{ K }[/math]. This entry will result in [math]\displaystyle{ E_p=K \sigma_{Y0} }[/math]. Softening will be unstable if is crosses entire cross section of a material under applied load, but is usually stable otherwise or when localized to a yield zone. To prevent non-physical negative values are large plastic strain, the softened yield stress must be limited to a minimum yield stress value (the default minimum is zero).

Hardening Law Properties

The material parameters in this hardening law are defined with the following properties:

Property Description Units Default
yield The initial yield stress. This stress corresponds to the axial stress at yield during uniaxial, 3D loading. pressure units Very Large
Ep The plastic modulus. This modulus is the slope of total stress as a function of plastic strain during uniaxial, 3D loading. The default of 0.0 results in an elastic-perfectly plastic material or a material with no hardening. It must be non-negative, but you can enter softening by using negative Khard. pressure units 0.0
Khard Alternatively, you can enter this dimensionless parameter for hardening. It is only used if Ep is not entered and when entered, it is convert to Ep using Ep = [math]\displaystyle{ \sigma_{Y0}K }[/math]. K can be positive (hardening) or negative (softening) pressure units 0.0
yieldMin The minimum yield stress. This minimum only matters when using negative Khard or when modeling softening plasticity pressure units 0

History Data

This hardening law defines one history variable, which is stored as history variable #1. It stores the the cumulative equivalent plastic strain (absolute) defined as

      [math]\displaystyle{ \alpha = \sum \sqrt{2\over3}\ ||d\varepsilon_p|| }[/math]

where dεp is the incremental plastic strain tensor in one time step.